Abstract
An equation for the electric current in a semiconductor space-charge region such as a p-n junction is derived. At low currents the equation has the usual form i=neμ*E−(q/e) μ*kTL∂n/∂x but the effective mobility μ* is shown to have a strong dependence on position and may be infinite or negative. This spatial dependence arises because the deviation of the average carrier energy from its equilibrium value has a first-order dependence on the current.

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